2008
DOI: 10.1364/oe.16.021315
|View full text |Cite
|
Sign up to set email alerts
|

Propagation of Bessel-Gaussian beams with optical vortices in turbulent atmosphere

Abstract: An approximate expression of a Bessel-Gaussian beam (BGB) with desired topological charge is introduced using a coherence superposition of decentered Gaussian beams (dGBs). And based on such an expression and the extended Huygens-Fresnel principle, the propagation properties of BGBs traveling in turbulent atmosphere are explored. An analytical expression of the average intensity of a BGB with phase singularity propagating through turbulent atmosphere is obtained and analyzed numerically. It is found that inten… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
30
0
2

Year Published

2009
2009
2023
2023

Publication Types

Select...
5
1
1

Relationship

0
7

Authors

Journals

citations
Cited by 130 publications
(32 citation statements)
references
References 25 publications
0
30
0
2
Order By: Relevance
“…The complex amplitude of a fundamental Bessel optical beam Eðx; RÞ at the observation point fx; Rg is described by a paraxial wave equation, where x is the distance between the source plane and the observation plane, and R is the vector that determines the distance between the observation point and the optical axis of the laser beam in a plane normal to the radiation propagation direction. Using the extended Huygens-Fresnel principle 12 for the secondorder mutual coherence function of the optical beam field, the mean field intensity of the fundamental Bessel optical beam propagating in a turbulent atmosphere can be written as [12][13][14][15]17 hIðx;RÞi¼hEðx;RÞE Ã ðx;RÞi…”
Section: Basic Determinationsmentioning
confidence: 99%
See 2 more Smart Citations
“…The complex amplitude of a fundamental Bessel optical beam Eðx; RÞ at the observation point fx; Rg is described by a paraxial wave equation, where x is the distance between the source plane and the observation plane, and R is the vector that determines the distance between the observation point and the optical axis of the laser beam in a plane normal to the radiation propagation direction. Using the extended Huygens-Fresnel principle 12 for the secondorder mutual coherence function of the optical beam field, the mean field intensity of the fundamental Bessel optical beam propagating in a turbulent atmosphere can be written as [12][13][14][15]17 hIðx;RÞi¼hEðx;RÞE Ã ðx;RÞi…”
Section: Basic Determinationsmentioning
confidence: 99%
“…In this regard, research of the features of propagation in a turbulent atmosphere for the Bessel and Bessel-Gaussian beams is vigorously performed. [13][14][15][16][17][18][19][20][21] The majority of these works [13][14][15][16][17] is devoted to the analysis of various aspects of the behavior of the mean intensity of coherent 13,16,17 and partially coherent 14 BesselGaussian beams in randomly inhomogeneous media. In these researches, special attention is given to preservation consideration (or changes) during the propagation of topological structure of Bessel-Gaussian beams.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…0 2 0 2 0 0 gb P E a P = π ≅ (12) Considering expression (12), we will notice, that data for mean intensity of a Gaussian optical beam with a vortex phase factor ( ) …”
Section: Mean Intensity Of Gaussian Optical Beam With Vortex Phase Famentioning
confidence: 99%
“…[1][2][3][4][5] However, till now propagation of vortex optical beams usually examine either in a homogeneous medium, or in a turbulent (randomly inhomogeneous) atmosphere. [6][7][8][9][10][11][12][13][14][15][16][17] Other types of the randomly inhomogeneous media, in particular the discrete scattering media, while remain out of sight of researchers. Meanwhile, in media of propagation of optical radiation often there are particles of matter which actively participate in light scattering.…”
Section: Introductionmentioning
confidence: 99%